Download Experiment 6 Newton`s Second Law A mass is allowed to fall

Experiment 6
Newton's Second Law
A mass is allowed to fall vertically while pulling another mass over a horizontal surface.
The motion of the system is investigated, and the application of Newton's Second Law to the
system allows the determination of the acceleration of the system.
Theory
Newton's Second Law states that the resultant of the forces acting on a body to accelerate in
the direction of the resultant force. This can be expressed mathematically as


 F = ma ,
(1)
where m is the mass of the body and a is its acceleration. When expressed in terms of the force
components,
 F x = m ax ;  F y = m a y ,
(2)
where a x and a y represent the x and y components of the acceleration.
In this experiment, a body of mass m1 falls vertically. One end of a string is attached to
m1 . The other end is attached to a body of mass m2 which is pulled along the surface of the air
track. (Refer to Figure 1.) The string passes over a pulley that is of very low mass and practically
frictionless. Because of this, the effect of the pulley on the system can be neglected.
Figure 1. The air track with the first mass moving downward and pulling the second
over the surface of the air track.
1
When Newton's Second Law is applied to the two bodies, the acceleration of the system is
g
a = m1
.
m1 + m2
(3)
Apparatus
o
o
o
o
air track with air supply and sparker
glider
o spark tape
meter stick
o masking tape
hanging masses
o masses to be attached to glider
The air tracks have been leveled. Please do not move them.
Procedure
1) Use masking tape to attach a one meter length of spark tape to the pulley end of the
yellow-colored mounting strip on the air track.
Group
Number
m1
(grams)
mass added to
glider (grams)
Timing Interval
(sec)
1
12
0
1/6
2
13
0
1/6
3
14
0
1/6
4
15
100
1/6
5
16
100
1/6
6
17
100
1/6
7
18
100
1/6
8
19
200
1/6
9
20
200
1/6
10
21
200
1/6
Figure 2.
Mass values for the hanging mass and the mass to be added to
the glider.
2) Attach the amount of mass corresponding to your group number to the glider. (Refer to
2
Figure 2.) Be sure to equally distribute the total mass to both sides of the glider.
Record the mass of the glider and the total mass added to the glider. This mass is m2.
3) Carefully place the glider on the air track. Pass the string over the pulley and attach to
the end of the string the amount of mass listed for your group number.
4) Turn on the air supply. (The air flow is adjusted high enough so that the glider floats
above the surface of the track.) Set the spark timer to the proper frequency. Prevent the
glider from moving by placing your finger on the air track in front of the glider.
5) Start the spark timer, then release the glider. Keep the spark timer engaged until the
glider reaches the end of the air track.
6) Carefully remove the spark tape and affix it on a flat surface with making tape. Cross
out the dot corresponding to the starting position. Circle the remaining dots and number
the dots successively. Place the meter stick on the tape and record the position of each
dot. A suggested form for the table for each set of data is shown in Figure 3.
data
point
time, multiples
of t
distance,
s
change in
distance, s
average
velocity
1
0
s1
2
1.00
s2
s3 - s1
( s3 - s1 )/ 2t
3
2.00
s3
s4 - s 2
( s4 - s2 )/ 2t
4
3.00
s4
s5 - s3
( s5 - s3 )/ 2t
(etc.)
Figure 3. A suggested form for the data table.
Analysis
Draw free-body diagrams for the two masses, m1 and m2 . Apply Newton's Second Law
and derive (3).
Complete the calculations of the average velocities for the data. First calculate the distance
from one data point to the second data point away, s . Then find the average velocity by dividing
s by the time taken to travel that distance, 2t , which is twice the park timing interval. Because
the acceleration is constant, the average velocity is numerically equal to the instantaneous velocity
at the point halfway in time between the data points.
3
Graph the values of instantaneous velocity versus time, with velocity as the ordinate and
time as the abscissa. Draw two lines that best fit the data: one with maximum slope, a max , and one
with minimum slope, a min . Find the slopes of these lines. The best value for the acceleration of the
system is then
1
a = ( a max + a min ) ,
2
(4)
and the corresponding uncertainty in the acceleration is
1
a = ( a max - a min ) .
2
(5)
Calculate the best value for the acceleration, (4) and the uncertainty, (5).
On a one-dimensional graph, use points and error bars to plot a + _ a . Be sure to displace
vertically the error bar from the axis so that it is clearly visible. Now calculate the theoretical value
of the acceleration from (3) and plot it on the graph described above so that the point is displaced
slightly above the error bar.
Report in a results table, a + _ a and the theoretical value of a .
Conclusions
Indicate what the major sources of error are, and explain how the experimental values are
affected by these sources of error. Explain whether or not the experimental value of the
acceleration shows the effects of the sources of error.
Questions
1) If friction is present between the glider and the air track, then how will the experimental
value of the acceleration be different from the theoretical value? Explain why. Do the
results indicate the presence of friction? Explain.
2) If the mass of the pulley is not negligible, then how will the experimental value of the
acceleration be different from the theoretical value? Explain why.
3) If the experimental value of the acceleration is greater than the theoretical value, then
what is the most likely reason for this?
4